Abstract:
A particle diameter measuring device for measuring the particle diameter distribution of a number of particles to be measured, wherein a laser beam guided through a radiating optical fiber is re-formed by collimator lenses into parallel beams having an adequate diameter and is then irradiated onto the particles to be measured; a plurality of optical fibers are arranged along a circle whose center is a point P located in the particles, the receiving end of any of the optical fibers being directed toward point P. The optical fibers receiving the scattered light are arranged close to one another in the range of small scattering angles, while they are roughly arranged in the range of large scattering angles. A transmitted light enters into that optical fiber which is so arranged as to coincide with the laser beam incident direction, the intensity of this transmitted light being detected by a photodetector. Light scattered at various angles, which angles are formed with reference to the laser beam incident direction, is received by the other optical fibers, their intensities being detected by the other photo-detectors. The transmission factor t=Iout/Iin in calculated from the intensity of the transmitted light. The particle diameter distribution n(D) is calculated in the form of relative values, using the angular distribution I(.theta.) of the scattered light intensity. The particle diameter distribution N(D) is calculated in the form of absolute values, using t, n(D) and light pass length L. On the while, particle diameter distribution N(D) or n(D) can be measured with high accuracy, independently of the diameter of the particles. Since it is easy to measure the scattered light intensities in a range of scattering angles from 0.degree. to 30.degree., the particle diameter distribution of particles, the diameter thereof are smaller than 0.1 .mu.m, can be obtained.
Abstract:
An optical fiber sensor, which has a detector section connected in a single optical path made of an optical-fiber cable and having a light-modulating element and an optical element connected in series. The light-modulating element has its birefringence degree changed in accordance with the physical quantity to be sensed, thereby to modulate the polarization state of the physical quantity. The optical element converts the polarization state of the physical quantity into the intensity of light. The sensor further comprises two light sources, which apply two light beams having different wavelengths .lambda..sub.1 and .lambda..sub.2 to one end of the optical path. The intensities P.sub.1 and P.sub.2 of the beams of the wavelengths .lambda..sub.1 and .lambda..sub.2, both emitted from the other end of the optical path, are detected. The intensities .lambda..sub.1 and .lambda..sub.2 vary in accordance with the changes in the intensity of the light emitted from the light sources, in the loss at the optical-fiber cable and the optical connector, and in the physical quantity to be detected. To obtain data free of the changes in the intensity of the light emitted from the light sources, in the loss at the optical-fiber cable and the optical connector, one type of the sensor has means for controlling one of the light sources such that the intensities P.sub.1 and P.sub.2 are at the same level, and means for detecting the intensities P.sub.01 and P.sub.02 of the light beams emitted from the two light sources and performing the calculation of (P.sub.01 -P.sub.02)/(P.sub.01 +P.sub.02).
Abstract:
A temperature measuring device intended to use the photoelastic effect of a transparent element. The present invention employs as the temperature sensing element a thermal expansion photoelastic cell comprising a photoelastic element and a stress generating element which are closely contacted with each other for yielding stress of anisotropy in the photoelastic element, which changes in response to changing ambient temperature, as the stress generating element is quite remarkably different in thermal expansion coefficient from the photoelastic element. An element is further provided to detect phase difference between two orthogonal light components passed through the photoelastic element which are one polarized component in a stress direction and the other component polarized in a direction perpendicular to the above stress direction when linearly polarized light is passed through the photoelastic element of the thermal expansion photoelastic cell. The detected phase difference is converted into a temperature, which is then displayed on a display device.
Abstract:
A registration system for registering a target registration object with respect to a predetermined reference position by using a registration mark formed on the target registration object includes the intensity measurement step of receiving a mark image for a predetermined period of time by a storage type sensor while an area of the target registration object which includes the mark is illuminated, the storage type sensor having elements whose positional relationship is known with respect to the mark image, the process of obtaining a center position of the mark image on the storage type sensor in a positioning direction in accordance with outputs from the elements of the storage type sensor obtained in the intensity measurement step, the distance calculation step of calculating a distance between the reference position and the center position obtained by the process, and the moving step of moving the target registration object by a distance corresponding to the distance obtained in the distance calculation step.
Abstract:
An optical system for irradiation comprising a light source, a lens, an optical fiber, a rectangular waveguide, an objective lens and a prism and an optical system for receiving light comprising an objective lens, an aperture and an optical fiber are arranged with their optical axes intersecting one another at a point P in a measuring volume. In the optical system for irradiation, the light emitted from the optical fiber and having an intensity distribution expressed by a normal distribution curve is changed to a light having a uniform intensity distribution and a rectangular cross section, which is irradiated through the prism to the point p in the measuring volume. A light scattered at an angle of 90.degree. by a particle flowing through the measuring volume is guided through the optical system for receiving light to a photodetector which converts the scattered light to an electric signal (current) called a scattered light pulse. An arithmetic unit calculates the particle size from the height of this scatterd light pulse and the flow speed from the pulse width.
Abstract:
A particle size measuring apparatus irradiates a number of particles to be measured with a laser beam, measures a light intensity pattern scattered by the particles to be measured, and calculates a relative particle size distribution of the particles to be measured from the measured value obtained. The apparatus has a laser unit, a collimator lens for collimating a laser beam from the laser unit into a parallel laser beam and irradiating the particles to be measured with the parallel laser beam, an optical shield, interposed between the collimator lens and the particles to be measured, for shielding scattered light by the collimator lens and allowing passage of only parallel components of the laser beam, a detecting section consisting of a plurality of optical fibers arranged at an equal distance from a measurement region and at predetermined scattering angles and photodetectors connected thereto, and an arithmetic operating circuit for calculating a relative particle size distribution of the particles to be measured from the scattered light intensity pattern detected by the detecting section.
Abstract:
A droplet size measuring apparatus of the forward scattering method, wherein particles to be measured in a scattering zone having a predetermined scattering path length are irradiated with parallel laser beams. The irradiated beams are scattered by the particles and the scattering beams are detected by the photodetectors arranged at predetermined scattering angles. The output of the photodetectors are input to an arithmetic operating unit, thus the intensity distribution I(.theta.) of the scattered beams is measured. The droplet size distribution n(D) is calculated from the intensity distribution I(.theta.) using the following equation:I(.theta.)=.intg.{I.sub.0 exp(-l.intg.c(D)n(D)dD..intg.i(D,.theta.+.theta..sub.l)n(D)d(D)}dl
Abstract translation:前向散射法的液滴尺寸测量装置,其中在具有预定散射路径长度的散射区域中被测量的颗粒被照射平行激光束。 照射的光束被颗粒散射,并且散射光束以预定散射角布置的光电检测器被检测。 光电检测器的输出被输入到算术运算单元,因此测量散射光束的强度分布I(θ)。 使用以下等式从强度分布I(θ)计算液滴尺寸分布n(D):I(θ)= INTEGRAL {I0 exp(-l INTEGRAL c(D)n(D)dD。INTEGRAL i ,θ+θl)n(D)d(D)} dl